Technical Field
[0001] This invention relates to methods and means for detecting focus errors in optical
heads adapted to read and write data on optical recording media, and more particularly
relates to improved means for generating a focus error signal for use as input to
a servo system operative to keep an optical beam in focus on a surface.
Background of the Invention
[0002] Focus-error detection methods heretofore used for optical storage applications generally
employ a knife edge, an astigmatic lens or a critical angle prism. These techniques
require very critical alignment of these optical elements and of a split or segmented
photodetector.
[0003] Published European patent application EP 0164687 discloses a detection technique
wherein a laser beam reflected from an optical disk is directed through an objective
lens to a prism that reduces beam width in one dimension by a factor M and delivers
an elliptical beam to a knife-edge-type focus error detection system. This application,
following equation (25), claims to increase the focus error signal by a factor of
M.
[0004] The Digest of the Topical Meeting on Optical Data Storage, October 15-17, 1985 at
Washington, D.C., includes Paper THCC2-1 by Yamamoto et al. entitled "Design Considerations
of Optical Pregroove Dimension". This paper shows a six-element photodetector to detect
the far field spot size variations associated with a focus error.
[0005] There is a need for a very sensitive focus-error detection technique that will provide,
with relatively few components, a significant enhancement of the focus-error signal
and provide a large beam size that only requires an uncritical alignment of a segmented
photodetector in one dimension.
Summary of the Invention
[0006] The present invention is defined in the attached claims.
[0007] Toward this end and according to the invention, an apparatus and method are provided
for detecting focus errors in an optical head by positioning a prism in the optical
path of a return light beam reflected from an optical recording medium. The prism
reduces the beam in one dimension by a factor of M and concurrently increases the
divergence/convergence angle associated with a focus-error of the beam by a factor
of M in said dimension, thereby desirably enhancing the focus error signal by a factor
of M². A focus error is detected by a segmented photodetector having inner and outer
photosensitive regions, such as shown in the Yamamoto et al. paper. The photodetector
generates an electrical signal indicative of the focus error from the difference in
light intensities at the inner and outer regions. The photodetector preferably is
segmented in such manner as to also provide a track error signal.
Brief Description of the Drawings
[0008]
Fig. 1 is a schematic diagram that illustrates the principle of the invention;
Figs. 2A and 2B illustrate two preferred configurations of a segmented photodetector,
both of which generate a focus error signal and Fig. 2B of which additionally generates
a track error signal;
Fig. 3 illustrates an optical head according to one embodiment of the invention for
use with read-only, write-once or phase-change optical disks;
Fig. 4 illustrates an embodiment for use with an optical disk drive employing a swing-arm
actuator; and
Fig. 5 illustrates an embodiment for use with magneto-optic disks.
Description of Preferred Embodiments
General
[0009] The principle of the invention is best illustrated in Fig. 1. The output of a diode
laser 10 is passed through a circularizer/collimator system 11 to provide a collimated
beam 12. On reflection from a beam splitter 13, beam 12 becomes beam 14. Beam 14 is
focused by a lens 15 onto surface 16 of an optical recording medium. When surface
16 is at the focus of lens 15, the collimated beam 14 from beam splitter 13 to lens
15 is retroreflected on itself and, as return beam 14, is transmitted by beam splitter
13 to a prism 17. Prism 17 refracts beam 14 as beam 18, which is directed to a photodetector
19. Beam 18 has an intensity pattern of elliptical configuration, with a major axis
equal to D and a minor axis A. Prism 17 reduces the width of beam 14 by a factor of
M (which is defined as D/A) to that of refracted beam 18.
[0010] Assume now that the data on surface 16 is out of focus by an amount δz. Under this
assumed condition, the beam 14′ reflected from surface 16 will, after passing through
lens 15, diverge with an angle δϑ, in which
δϑ = Dδz/f² (1)
where f is the focal length of lens 15.
[0011] If δz is negative, then δϑ will be negative and the beam 14′ will converge. The following
analysis considers the case of δz being positive, but when δz is small, the same analysis
is valid for a diverging or converging beam 14′.
[0012] The refracted beam 18′ emerging from prism 17 has a divergence angle of Mδϑ; and
the width A′ of said beam on detector 19 is now given by
A′ ≃ A + 2lMδϑ (2)
where l is the distance from prism 17 to photodetector 19.
[0013] Using equation (1), one obtains
A′ ≃ A + 2lMDδz/f²
≃ A + 2lm²Aδz/f²
or
A′/A ≃ 1 + 2lM²δz/f² (3)
[0014] It will thus be seen that, by inserting prism 17 in the path of the return beam 14′
from surface 16, the change in beam width A indicative of a focus error δz is enhanced
by a factor M². M is determined by the apex angle of prism 17, and by the refractive
index of the material from which it is made. M may be made arbitrarily large; however,
the tolerance on alignment of the system becomes increasingly tight as M increases.
A practical maximum value for a single prism 17 is approximately M=5; however, several
prisms may be used in series and the resultant factor M would then be the product
of the values of M for each prism.
[0015] As illustrated in Fig. 2A, photodetector 24 comprises three photosensitive striped
areas 1,2,3. Let I₁,I₂,I₃ be the electrical signals generated by the light incident
on these photosensitive areas 1,2,3, respectively. For the configuration shown in
Fig. 2A, let S₁ = I₁+I₃ and S₂ = I₂. Let kA be the width of central photosensitive
area 2 where k(≃0.25) is chosen such that S₁=S₂ when beam 14 is in focus. If S

and S

are the signals corresponding to a focus error δz, it can be shown that

When A′≃A and k=0.25,
FES ≃ 0.67(A′/A-1) ≃ 1.3lM²δz/f²
Thus, by way of example, if M=5, l=50 mm and f=4 mm, then a small focus error δz=0.5
µm gives a focus error signal FES=0.05. This large error signal will allow detection
of very small focus errors with high signal-to-noise ratio.
[0016] Signals I₁ and I₃ are summed and amplified at 20 to provide output signal S₁, whereas
signal I₂ is amplified at 21 to provide output signal S₂. Signals S₁ and S₂ are supplied
to a differential amplifier 22 and a summing amplifier 26 whose outputs are supplied
to divider circuit 28. The output of the divider circuit 28 is the focus error signal,
FES. The focus error signal is applied to a focus servo control system 23 (Fig. 1).
As illustrated, system 23 comprises conventional means (not shown) for adjusting the
current in a coil 24 for thereby adjusting the position of lens 15 relative to surface
16.
[0017] The preferred configuration of photodetector is shown in Fig. 2B. Photodetector 25
includes six photosensitive areas 1-6 for generating electrical signals I₁-I₆, respectively.
The focus error signal is given by

and the track error signal by

where
S₁ = I₁ + I₃ + I₄ + I₆
S₂ = I₂ + I₅
S₃ = I₁ + I₂ + I₃
S₄ = I₄ + I₅ + I₆
[0018] The manner in which the track error signal is used to adjust track error is conventional
and forms no part of the present invention. Fig. 2B is included merely to show that
applicants' method and means for detecting and correcting focus errors is compatible
with and desirably used in conjunction with a photodetector like 25 that generates
both focus error and track error signals.
Fig. 3
[0019] As illustrated in Fig. 3, the invention according to this embodiment comprises an
optical head especially suitable for use with read-only, write-once or phase-change
optical disks. A laser 30 emits a beam that is collimated by a lens 32 and circularized
by refraction at surface 34 of a prism 46. Surface 34 has a polarizing beam splitter
(PBS) coating. The beam 35 is directed through a quarter-wave plate 36 to a beam bender
38 and a lens 40 that focuses said beam onto a selectable track on an optical disk
42. The beam 35′ reflected from disk 42 returns through the wave plate 36 and is reflected
as beam 37 from surface 34 toward surface 44 of prism 46. Refraction of beam 37 at
surface 44 reduces the width of said beam by a factor of M from D to A and directs
this elliptical beam 47 to a photodetector 48 that preferably is segmented as shown
in Fig. 2A or 2B.
[0020] If, as illustrated in Fig. 3, the data on the track of disk 42 is in focus, then
the return beam 35′ will coincide with the beam 35, and the beam width at the photodetector
48 will be equal to A. If, however, the data on disk 42 is out of focus, then the
return beam 35′ will diverge from 35, and as illustrated in Fig. 1, cause the width
of the beam to the photodetector 48 to be greater than A. As described in connection
with Fig. 2, photodetector 48 will generate a FES; and the position of lens 40 relative
to the tracks on the disk 42 will be adjusted in response to this FES by suitable
servo means (not shown) as necessary to put the data in focus.
[0021] This embodiment requires a desirably low number of components.
Fig. 4
[0022] Figs. 4A and 4B illustrate another embodiment of an optical head for use with read-only,
write-once or phase-change disks. According to this embodiment, the general orientation
of the head is parallel to the tracks on a disk 50. This head is therefore most easily
adapted to a disk drive that employs a swing-arm actuator. A laser 52 (Fig. 4A) emits
a beam that is collimated by a lens 54 and directed to and through a PBS 56 without
deflection or reflection. Beam 58 from PBS 56 is elliptical in cross section, with
a width D in one dimension and a width A in a direction orthogonal thereto. This beam
58 passes through a quarter-wave plate 60 and is directed to a prism assembly 62.
At a first surface 64 of prism assembly 62, beam 58 is circularized, then reflected
by total internal reflectance (TIR) from another surface 66 to and off a reflective
surface 68 to an objective lens 70 that focuses the resultant beam 72 onto the disk
50. Beam 72 is reflected from a disk track as reflected beam 58′. Beam 58′, which
again is elliptical in cross section, is reflected by a surface 74 of the PBS 56 and
directed to a photodetector 76 that preferably is segmented as shown in Fig. 2A or
2B.
[0023] If, as illustrated in Fig. 4, the data on the track of disk 50 is in focus, then
the return beam 58′ will coincide with the beam 58, and the beam width at the photodetector
76 will be equal to A. If, however, the data on disk 50 is out of focus, then the
return beam 58′ will diverge from 58, and as illustrated in Fig. 1, cause the width
of the beam to the photodetector 76 to be greater than A. As described in connection
with Fig. 2, photodetector 48 will generate a FES; and the position of lens 70 relative
to the tracks on the disk 50 will be adjusted in response to this FES by suitable
servo means (not shown) as necessary to put the data in focus.
[0024] This embodiment requires that the expansion/compression ratio M of prism 66 must
be matched to the emission pattern of laser 52.
Fig 5
[0025] Fig. 5 illustrates still another embodiment of an optical head for use with magneto-optic
disks. A laser 80 emits a beam that is collimated by a lens 82, circularized by refraction
at surface 84 of a prism 86 and directed towards a beam bender 88 and an objective
lens 90. Surface 84 is a partially polarizing beam splitter surface that directs a
fraction of the p-polarized component of beam 92′ as reflected from a selected track
on disk 94, and substantially all of the s-polarized component of said beam to surface
98 of a prism 96 as a beam 100. Surface 98 is also a partially-polarizing beam splitter
surface. Surface 98 refracts a fraction of the p-polarized component of beam 100 as
a beam 101 to a servo photodetector 102 preferably segmented as shown in Fig. 2A or
2B. This refraction causes a reduction in one dimension of beam 100 by a factor of
M from D to A. Surface 98 also directs a fraction of the p-polarized component of
beam 100 as well as substantially all of the s-polarized component of beam 100 as
a beam 103 to a Wollaston prism 104, converging lens 106 and data detector 108. The
function of the Wollaston prism in detecting the data on a magneto-optic disk is well
known in the art and does not form part of the present invention.
[0026] If, as illustrated in Fig. 5, the data on the track of disk 94 is in focus, then
the return beam 92′ will coincide with the primary beam 92, and the beam width at
the photodetector 102 will be equal to A. If, however, the data on disk 94 is out
of focus, then the return beam 92′ will diverge from 92, and as illustrated in Fig.
1, cause the width of the beam to the photodetector 102 to be greater than A. As described
in connection with Fig. 2, photodetector 48 will generate a FES; and the position
of lens 90 relative to the tracks on the disk 94 will be adjusted in response to this
FES by suitable servo means (not shown) as necessary to put the data in focus.
[0027] It will now be seen that, in each of the configurations shown in Figs. 3-5, unlike
those taught by the prior art, the focus error signal is desirably enhanced by a factor
of M².
1. An apparatus for detecting focus errors in an optical head adapted to read and/or
write data on an optical recording medium (16), comprising:
a photodetector (19) for generating an electrical signal in response to a focus error;
and
at least one prism (17) positioned in the optical path of a return light beam (14)
reflected from said medium for reducing the beam in one dimension by a factor of M
and concurrently increasing the divergence/convergence angle associated with a focus
error of said beam by the factor of M in said dimension, thereby enhancing the focus
error signal by a factor of M².
2. The apparatus of claim 1, wherein said photodetector has inner and outer photosensitive
regions and generates the electrical signal from the difference in light intensities
at said inner and outer regions.
3. The apparatus of claim 2, wherein one inner region is centered between two outer
photosensitive regions such that the focus error signal generated is zero when the
intensity of the light detected at the inner region equals the sum of the light intensities
detected at both outer regions.
4. The apparatus of claim 2, wherein said photodetector has an inner photosensitive
region in the form of a stripe between two outer photosensitive regions and said regions
are divided in a direction perpendicular to the stripe to create three upper and three
lower photosensitive areas from which another electrical signal indicative of track
error is generated from the difference in light intensities of said upper and lower
areas.
5. The apparatus of claim 1, including:
means for providing a primary beam of collimated light; and
a focusing lens that directs said primary beam onto the medium, such that the return
beam coincides with the primary beam when said lens is in focus on the medium.
6. The apparatus of claim 5, including:
means, including servo means, responsive to the focus error signal resulting from
a divergence or convergence of the return beam from the primary beam indicative of
a focus error for adjusting the relative position of the lens and medium as necessary
to eliminate the focus error.
7. The apparatus of any of the claims 1-6, wherein the optical head is used with an
optical disk having a plurality of tracks for storing data, said head comprising:
prism means including a polarizing beam splitter for circularizing the beam by refraction;
and
means including a quarter-wave plate, beam bender and lens to focus the circularized
beam on a selected track.
8. The apparatus of claim 1, further comprising:
means for providing collimated light;
a quarter-wave plate;
said prism having one surface for circularizing the light transmitted through the
quarter-wave plate, a second surface from which the circularized light is reflected
by total internal reflectance, and a third surface which is reflective;
lens means for focusing the beam reflected from said third surface onto the disk;
and
a polarizing beam splitter for directing said return beam emitted by said prism means
to the photodetector.
9. The apparatus of claim 1, further comprising:
means for providing a beam of collimated light;
first prism means for circularizing the beam by refraction;
means including a beam bender and lens means via which the circularized beam is directed
to a selected track on the disk;
second prism means;
said first prism means having a partially polarizing beam splitter surface for directing
a fraction of the p-polarized component of the return beam reflected from the disk
and substantially all of the s-polarized component of said return beam to said second
prism means; and
a photodetector for generating a signal in response to a focus error of said return
beam;
said second prism means having a partially-polarizing beam splitter surface for refracting
a fraction of the p-polarized component of the last-named beam to said photodetector
for causing the last-named fraction to constitute a reduction of the return beam in
one dimension by a factor of M and concurrently increasing the divergence/convergence
angle associated with a focus error of said beam by a factor M in said dimension,
thereby enhancing said signal by a factor of M².
10. A method for detecting focus errors in an optical head to which a light beam is
directed for reading and/or writing data on an optical recording medium, comprising:
positioning a prism in the optical path of the return light beam reflected from said
medium for reducing the beam in one dimension by a factor of M and concurrently increasing
the divergence/convergence angle associated with a focus error of said beam by the
factor of M in said dimension for enhancing an electrical signal indicative of a focus
error by a factor of M².
11. The method of claim 10, including the further step of:
providing a photodetector having inner and outer photosensitive regions for generating
said signal from the difference in light intensities at said inner and outer regions.
12. The method of claim 11, wherein said regions are divided in a direction perpendicular
to the stripe to create three upper and three lower photosensitive areas each electrically
isolated from the other, and another electrical signal indicative of track error is
generated from the difference in light intensities of said upper and lower areas.
13. The method of claim 11, including the further step of adjusting the position of
a focusing lens within the optical path in response to said signal as necessary to
maintain the light intensity detected at said inner region equal to the sum of the
light intensities detected at said outer regions and thereby eliminate said focus
error.